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https://scholarbank.nus.edu.sg/handle/10635/91629
DC Field | Value | |
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dc.title | Photoconductivity in poly[[o-(trimethylsilyl)phenyl]acetylene] | |
dc.contributor.author | Kang, E.T. | |
dc.contributor.author | Neoh, K.G. | |
dc.contributor.author | Masuda, T. | |
dc.contributor.author | Higashimura, T. | |
dc.contributor.author | Yamamoto, M. | |
dc.date.accessioned | 2014-10-09T08:20:22Z | |
dc.date.available | 2014-10-09T08:20:22Z | |
dc.date.issued | 1989-07 | |
dc.identifier.citation | Kang, E.T.,Neoh, K.G.,Masuda, T.,Higashimura, T.,Yamamoto, M. (1989-07). Photoconductivity in poly[[o-(trimethylsilyl)phenyl]acetylene]. Polymer 30 (7) : 1328-1331. ScholarBank@NUS Repository. | |
dc.identifier.issn | 00323861 | |
dc.identifier.uri | http://scholarbank.nus.edu.sg/handle/10635/91629 | |
dc.description.abstract | Steady-state photoconductivity was studied in thin films of poly[[o-(trimethylsilyl)phenyl]acetylene], or poly(o-Me3SiPA) sandwiched between SnO2 and metal electrodes. Both the dark current density (Jd) and photocurrent density (Jph) depend superlinearly on the applied electric field. Jph also shows a superlinear dependence on light intensity. However, Jd and Jph are only weak functions of temperature at temperatures below room temperature. We conclude that the photoconductivity in poly(o-Me3SiPA) arises mainly from trap-modulated carrier photoemission from electrodes and the polymer is capable of effective transport of holes. © 1989. | |
dc.source | Scopus | |
dc.subject | hole transport | |
dc.subject | photoconductivity | |
dc.subject | poly[[o-(trimethylsilyl)phenyl]acetylene] | |
dc.subject | thin film | |
dc.type | Article | |
dc.contributor.department | CHEMICAL ENGINEERING | |
dc.description.sourcetitle | Polymer | |
dc.description.volume | 30 | |
dc.description.issue | 7 | |
dc.description.page | 1328-1331 | |
dc.description.coden | POLMA | |
dc.identifier.isiut | NOT_IN_WOS | |
Appears in Collections: | Staff Publications |
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